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Density matrix functional theory in average and relative coordinates

Manby, FR, Knowles, PJ, Lloyd, AW

Published Jan 1, 2001• 0 citations
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The detailed nature of the correlated first-order density matrix for the model atoms in the title for arbitrary interparticle interaction u(r12)u({r}_{12})u(r12​) is studied. One representation with contracted information is first explored by constructing the momentum density $\ensuremath{\rho}(\mathbf{p})$ in terms of the wave function of the relative motion, say ${\ensuremath{\Psi}}_{R}({r}_{12})$, which naturally depends on the choice of u(r12)u({r}_{12})u(r12​). For u(r12)=e2∕r12u({r}_{12})={e}^{2}∕{r}_{12}u(r12​)=e2∕r12​, the so-called Hookean atom, and for the inverse square law $u({r}_{12})=\ensuremath{\lambda}∕{r}_{12}^{2}$, plots are presented of the above density $\ensuremath{\rho}(\mathbf{p})$ in momentum space. The correlated kinetic energy is recovered from averaging p2∕2m{p}^{2}∕2mp2∕2m, mmm denoting the electron mass, with respect to $\ensuremath{\rho}(\mathbf{p})$. The second method developed is in coordinate space and expands the density matrix $\ensuremath{\gamma}({\mathbf{r}}_{1},{\mathbf{r}}_{2})$ in Legendre polynomials, using relative coordinate ${\mathbf{r}}_{1}\ensuremath{-}{\mathbf{r}}_{2}$, center-of-mass coordinate (r1+r2)∕2({\mathbf{r}}_{1}+{\mathbf{r}}_{2})∕2(r1​+r2​)∕2 and the angle, $\ensuremath{\theta}$ say, between these two vectors. For the Moshinsky atom in which u(r12)=12kr122u({r}_{12})=\frac{1}{2}k{r}_{12}^{2}u(r12​)=21​kr122​ only the sss term (l=0)(l=0)(l=0) contributes to the Legendre polynomial expansion. The specific example we present of the inverse square law model is shown to be characterized by the low-order terms (s+d)(s+d)(s+d) of the Legendre expansion. The Wigner function is finally calculated analytically for both Moshinsky and inverse square law models.